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crc press - E-Lib FK UWKS

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Interactions of Cell-Penetrating Peptides with Membranes 171<br />

FIGURE 8.1 Variations of the surface <strong>press</strong>ure with the mean molecular area of mixed<br />

DOPC- 1 monolayers at various peptide molar fractions (x P). (Adapted from Van Mau, N. et al.,<br />

J. Membr. Biol., 167, 241, 1999. With permission.)<br />

of the membrane uptake of this peptide was undertaken using mainly monolayers<br />

AFM and FTIR. 57,58<br />

8.2.2.8.1 Monolayer Study<br />

Because of its solubility properties, the peptide could be dissolved in the same<br />

volatile organic solvent mixture as the phospholipids (DOPC, DOPG, DPPC, and<br />

DPPG) and, hence, the peptide–lipid mixtures could be spread at the air–water<br />

interface. The various com<strong>press</strong>ion isotherms at various peptide molar fractions were<br />

recorded and are shown in Figures 8.1 and 8.2.<br />

Analysis of the isotherm was made by plotting the variation of the mean molecular<br />

area as a function of the molar fraction at a given surface <strong>press</strong>ure. In all cases<br />

the variations of the mean molecular area showed positive deviations from additivity<br />

(Figure 8.3 and insets of Figure 8.2). 109,110 Such behavior can be considered indicative<br />

of strong peptide–lipid interactions with expansion of the mean molecular area.<br />

However, the deviation from linearity is larger in DOPC and DOPG than in DPPC<br />

and DPPG, suggesting that the nature of the peptide–lipid interactions could strongly<br />

depend on the nature of the fatty acid. Further investigations, based now on FTIR,<br />

showed clearly that the peptide underwent a conformational transition, going from<br />

an α-helical form at low peptide molar fraction to a β-type structure at higher molar<br />

fractions. This conformational transition was detected by examination of the position<br />

of the Amide I band, the major component of which moves from 1655 cm –1 (wavenumber<br />

characteristic of an α-helix) to 1625 cm –1 (wavenumber characteristic of a<br />

sheet structure) 111,112 upon increasing the peptide molar fraction (Figure 8.4). This<br />

holds true, at least, when the peptide interacts with DOPG, but probably also for<br />

DOPC. However, a transition occurs at very low peptide molar fractions, probably

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